/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 30 Suppose that an ideal capacitor ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Suppose that an ideal capacitor and an ideal inductor are connected in series in an ac circuit. (a) What is the phase difference between \(v_{\mathrm{C}}(t)\) and \(v_{\mathrm{L}}(t) ?\) [Hint: since they are in series, the same current \(i(t)\) flows through both. \(]\) (b) If the rms voltages across the capacitor and inductor are \(5.0 \mathrm{V}\) and \(1.0 \mathrm{V}\), respectively, what would an ac voltmeter (which reads rms voltages) connected across the series combination read?

Short Answer

Expert verified
Calculate the RMS voltage across the series combination of the capacitor and inductor, given the individual RMS voltages across each component. Answer: The phase difference between the voltage across the capacitor and the voltage across the inductor is \(\pi\) or 180 degrees. The RMS voltage across the series combination is approximately 5.10 V.

Step by step solution

01

Recall the voltage relations for capacitors and inductors in an AC circuit

In an AC circuit with sinusoidal voltage and current, the voltage across a capacitor is given by \(v_C(t) = V_C\sin(\omega t - \frac{\pi}{2})\) and the voltage across an inductor is given by \(v_L(t) = V_L\sin(\omega t + \frac{\pi}{2})\), where \(V_C\) and \(V_L\) are the peak voltages of the capacitor and inductor, respectively, \(\omega\) is the angular frequency, and \(t\) is time.
02

Determine the phase difference

Comparing the expressions for \(v_C(t)\) and \(v_L(t)\), we can see that the phase difference between the voltage across the capacitor and the inductor is \(\Delta \phi = \left(\frac{\pi}{2} + \frac{\pi}{2}\right) = \pi\) or 180 degrees. This means that the voltage across the capacitor and inductor are exactly out of phase with each other. #RMS Voltage Across the Series Combination#
03

Write expressions for RMS voltages

The given RMS voltages across the capacitor and inductor are 5.0 Volts and 1.0 Volts, respectively. Recall that the RMS voltage (\(V_\textrm{RMS}\)) is related to the peak voltage (\(V_\textrm{peak}\)) by the equation \(V_\textrm{RMS} = \frac{V_\textrm{peak}}{\sqrt{2}}\). This allows us to find the peak voltages across the capacitor and inductor: \(V_C = 5.0\sqrt{2}\) and \(V_L = 1.0\sqrt{2}\).
04

Determine the total peak voltage across series combination

Since the voltage across the capacitor and inductor are out of phase, we need to use the Pythagorean theorem to find the total peak voltage across the series combination, \(V_\textrm{total peak}\): $$V_\textrm{total peak} = \sqrt{V_C^2 + V_L^2} = \sqrt{(5.0\sqrt{2})^2 + (1.0\sqrt{2})^2}$$
05

Find the RMS voltage across the series combination

To find the RMS voltage across the series combination, we need to convert the total peak voltage to its RMS equivalent using the formula \(V_\textrm{RMS} = \frac{V_\textrm{peak}}{\sqrt{2}}\). $$V_\textrm{total RMS} = \frac{V_\textrm{total peak}}{\sqrt{2}} = \frac{\sqrt{(5.0\sqrt{2})^2 + (1.0\sqrt{2})^2}}{\sqrt{2}} \approx 5.10 \mathrm{V}$$ So the AC voltmeter connected across the series combination would read approximately 5.10 V.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A series combination of a resistor and a capacitor are connected to a \(110-\mathrm{V}\) rms, \(60.0-\mathrm{Hz}\) ac source. If the capacitance is \(0.80 \mu \mathrm{F}\) and the rms current in the circuit is $28.4 \mathrm{mA},$ what is the resistance?
A capacitor and a resistor are connected in parallel across an ac source. The reactance of the capacitor is equal to the resistance of the resistor. Assuming that \(i_{\mathrm{C}}(t)=I \sin \omega t,\) sketch graphs of \(i_{\mathrm{C}}(t)\) and \(i_{\mathrm{R}}(t)\) on the same axes.
In the crossover network of Problem \(61,\) the inductance \(L\) is $1.20 \mathrm{mH}$. The capacitor is variable; its capacitance can be adjusted to set the crossover point according to the frequency response of the woofer and tweeter. What should the capacitance be set to for a crossover point of $180 \mathrm{Hz} ?[\text {Hint}:$ At the crossover point, the currents are equal in amplitude. \(]\)
A large coil used as an electromagnet has a resistance of \(R=450 \Omega\) and an inductance of \(L=2.47 \mathrm{H} .\) The coil is connected to an ac source with a voltage amplitude of \(2.0 \mathrm{kV}\) and a frequency of $9.55 \mathrm{Hz}$. (a) What is the power factor? (b) What is the impedance of the circuit? (c) What is the peak current in the circuit? (d) What is the average power delivered to the electromagnet by the source?

A capacitor is connected across the terminals of a 115 \(\mathrm{V}\) rms, \(60.0-\mathrm{Hz}\) generator. For what capacitance is the rms current \(2.3 \mathrm{mA} ?\)

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.